Put , the velocity in the shock frame. The mass jump condition gives a common mass flux . Subtracting times the mass balance from the momentum balance gives
For energy, transform the conserved energy to the shock frame by subtracting times momentum and adding times mass. The resulting energy flux is
For a genuine shock, ; dividing its continuous energy flux by the same nonzero on both sides gives
The second term is the ideal-gas specific enthalpy. A contact discontinuity has zero relative mass flux and does not in general require equal specific enthalpies; the division here is appropriate for the shock specified in the question.

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